Problem 10
Question
A hockey puck with mass 0.160 \(\mathrm{kg}\) is at rest on the horizontal, frictionless surface of a rink. A player applies a force of 0.250 \(\mathrm{N}\) to the puck, parallel to the surface of the ice, and continues to apply this force for 2.00 \(\mathrm{s}\) . What are the position and speed of the puck at the end of that time?
Step-by-Step Solution
Verified Answer
The puck's position is 3.125 meters, and its speed is 3.125 m/s after 2 seconds.
1Step 1: Identify Given Values
We will start by identifying the given values in the problem. A mass of the puck: \( m = 0.160 \, \text{kg} \), a force applied: \( F = 0.250 \, \text{N} \), and the duration of force application: \( t = 2.00 \, \text{s} \). The initial velocity \( v_0 \) is 0 since the puck starts at rest.
2Step 2: Calculate the Acceleration
Use Newton's second law to find acceleration. According to the law, \( F = ma \). Therefore, acceleration \( a = \frac{F}{m} = \frac{0.250 \, \text{N}}{0.160 \, \text{kg}} = 1.5625 \, \text{m/s}^2 \).
3Step 3: Determine the Final Velocity
Use the equation of motion \( v = v_0 + at \) to calculate the final velocity. Since \( v_0 = 0 \), \( v = 0 + (1.5625 \, \text{m/s}^2)(2.00 \, \text{s}) = 3.125 \, \text{m/s} \).
4Step 4: Calculate the Final Position
Use the equation \( s = v_0 t + \frac{1}{2} at^2 \) to find the final position. Substituting the known values, \( s = 0 \times 2 + \frac{1}{2} \times 1.5625 \times 2^2 = 3.125 \, \text{m} \).
5Step 5: Summarize the Results
The final position of the puck is 3.125 meters, and the final speed is 3.125 meters per second after 2.00 seconds.
Key Concepts
Acceleration CalculationEquations of MotionForce and Mass Relationship
Acceleration Calculation
When understanding the movement of objects, calculating acceleration is crucial. Acceleration represents how an object's velocity changes over time. To find it, we use Newton's Second Law which connects force, mass, and acceleration with the formula: \[ F = ma \] Where:- \( F \) is the force applied, - \( m \) is the mass of the object, - \( a \) is the acceleration.In the case of the hockey puck, we know the force applied is \( 0.250 \, \text{N} \), and the puck's mass is \( 0.160 \, \text{kg} \). By rearranging the formula to solve for acceleration, we get\[ a = \frac{F}{m} \] Substituting the given values gives us:\[ a = \frac{0.250}{0.160} \approx 1.5625 \, \text{m/s}^2 \]This tells us how fast the puck's velocity is changing, or accelerating, as it is pushed along the ice.
Equations of Motion
Equations of motion allow us to predict the future movement of an object given its initial conditions and the forces acting on it. These equations incorporate information about time, velocity, acceleration, and displacement. For the hockey puck, we can use these equations to determine both the speed and position of the puck after the force is applied.
- The formula for final velocity \( v \) is based on initial velocity \( v_0 \), acceleration \( a \), and time \( t \):\[ v = v_0 + at \]Since the puck starts from rest, \( v_0 = 0 \), so:\[ v = 1.5625 \, \text{m/s}^2 \times 2 \, \text{s} = 3.125 \, \text{m/s} \]
- The equation to find the position \( s \) is:\[ s = v_0 t + \frac{1}{2} a t^2 \]Plugging in the values:\\[ s = 0 \times 2 + \frac{1}{2} \times 1.5625 \times 2^2 = 3.125 \, \text{m} \]
Force and Mass Relationship
The interplay between force, mass, and acceleration is foundational to Newton's Second Law. This relationship dictates how an object's velocity will change when a force is applied. Understanding this concept helps us predict how objects respond to different forces based on their mass.
- **Force**: Measured in newtons (N), it represents the push or pull exerted on an object.
- **Mass**: A scalar quantity that indicates how much matter is in an object, measured in kilograms (kg). It tells us how resistant an object is to acceleration when a force is applied.
- **Acceleration**: The rate of change of velocity that occurs when a force acts on mass. It's measured in meters per second squared (\( \text{m/s}^2 \)).
Other exercises in this chapter
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